Iraj Maleki Shahrivar, S. Mehdi Vaez Allaei, Shahab Naghavi
{"title":"聚碲方形平面链诱导的非谐波性使 Al2Te5 单层具有超低热导率和超高热电效率","authors":"Iraj Maleki Shahrivar, S. Mehdi Vaez Allaei, Shahab Naghavi","doi":"10.1039/d4cp01577k","DOIUrl":null,"url":null,"abstract":"Two-dimensional (2D) metal chalcogenides provide rich ground for the development of nanoscale thermoelectrics, although achieving optimal thermoelectric efficiency has yet to be a challenge. Here, we leverage the unique chemistry of tellurium (Te), renowned for its hypervalent bonding and catenation abilities, to tackle this challenge as manifested in Al<small><sub>2</sub></small>Te<small><sub>3</sub></small> and Al<small><sub>2</sub></small>Te<small><sub>5</sub></small> monolayers. While the former forms a straightforward covalent Al–Te network, the latter adopts a more intricate bonding mechanism, enabled by eccentric features of Te chemistry, to maintain charge balance. In Al<small><sub>2</sub></small>Te<small><sub>5</sub></small>, a square planar chain (SPC) known as polytelluride [Te<small><sub>3</sub></small>]<small><sup>2-</sup></small> is neutralized by covalently bonded [Al<small><sub>2</sub></small>Te<small><sub>2</sub></small>]<small><sup>2+</sup></small> framework. The hypervalent nature of Te results in bizarre Born effective charges of 7 and -4 for adjacent Te atoms within the square planar chain, the feature that induces significant anharmonicity, and leads to a glass-limit of lattice thermal conductivity (κ<small><sub>L</sub></small>) in Al<small><sub>2</sub></small>Te<small><sub>5</sub></small> monolayers. Enhanced anharmonic lattice vibrations and the accordion pattern bestow glass-like, strongly anisotropic thermal conductivity to the Al<small><sub>2</sub></small>Te<small><sub>5</sub></small> monolayer. The calculated κ<small><sub>L</sub></small> values of 1.8 and 0.5 Wm<small><sup>-1</sup></small>K<small><sup>-1</sup></small> along the a- and b-axes at 600 K are one order of magnitude lower than those of Al<small><sub>2</sub></small>Te<small><sub>3</sub></small>, and even lower than monolayers that contain heavy cations like Bi<small><sub>2</sub></small>Te<small><sub>3</sub></small>. Moreover, the tellurium chain dominates the valence band maximum and conduction band minimum of Al<small><sub>2</sub></small>Te<small><sub>5</sub></small>, leading to a high valley degeneracy of 10, and thus a high power factor and figure of merit (zT). Using rigorous first-principles calculations of electron relaxation time, the estimated hole-doped and electron-doped zT of, respectively, 1.5 and 0.5 at 600 K is achieved for Al<small><sub>2</sub></small>Te<small><sub>5</sub></small>. The pioneering zT of Al<small><sub>2</sub></small>Te<small><sub>5</sub></small> compared to that of Al<small><sub>2</sub></small>Te<small><sub>3</sub></small> is rooted merely in its amorphous-like lattice thermal transport and its polytelluride chain. These findings underscore the importance of aluminum telluride and polymeric-based inorganic compounds as practical and cost-effective thermoelectric materials, pending further experimental validation.","PeriodicalId":99,"journal":{"name":"Physical Chemistry Chemical Physics","volume":null,"pages":null},"PeriodicalIF":2.9000,"publicationDate":"2024-06-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Polytelluride square planar chain induced anharmonicity results in ultralow thermal conductivity and high thermoelectric efficiency in Al2Te5 monolayers\",\"authors\":\"Iraj Maleki Shahrivar, S. Mehdi Vaez Allaei, Shahab Naghavi\",\"doi\":\"10.1039/d4cp01577k\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Two-dimensional (2D) metal chalcogenides provide rich ground for the development of nanoscale thermoelectrics, although achieving optimal thermoelectric efficiency has yet to be a challenge. Here, we leverage the unique chemistry of tellurium (Te), renowned for its hypervalent bonding and catenation abilities, to tackle this challenge as manifested in Al<small><sub>2</sub></small>Te<small><sub>3</sub></small> and Al<small><sub>2</sub></small>Te<small><sub>5</sub></small> monolayers. While the former forms a straightforward covalent Al–Te network, the latter adopts a more intricate bonding mechanism, enabled by eccentric features of Te chemistry, to maintain charge balance. In Al<small><sub>2</sub></small>Te<small><sub>5</sub></small>, a square planar chain (SPC) known as polytelluride [Te<small><sub>3</sub></small>]<small><sup>2-</sup></small> is neutralized by covalently bonded [Al<small><sub>2</sub></small>Te<small><sub>2</sub></small>]<small><sup>2+</sup></small> framework. The hypervalent nature of Te results in bizarre Born effective charges of 7 and -4 for adjacent Te atoms within the square planar chain, the feature that induces significant anharmonicity, and leads to a glass-limit of lattice thermal conductivity (κ<small><sub>L</sub></small>) in Al<small><sub>2</sub></small>Te<small><sub>5</sub></small> monolayers. Enhanced anharmonic lattice vibrations and the accordion pattern bestow glass-like, strongly anisotropic thermal conductivity to the Al<small><sub>2</sub></small>Te<small><sub>5</sub></small> monolayer. The calculated κ<small><sub>L</sub></small> values of 1.8 and 0.5 Wm<small><sup>-1</sup></small>K<small><sup>-1</sup></small> along the a- and b-axes at 600 K are one order of magnitude lower than those of Al<small><sub>2</sub></small>Te<small><sub>3</sub></small>, and even lower than monolayers that contain heavy cations like Bi<small><sub>2</sub></small>Te<small><sub>3</sub></small>. Moreover, the tellurium chain dominates the valence band maximum and conduction band minimum of Al<small><sub>2</sub></small>Te<small><sub>5</sub></small>, leading to a high valley degeneracy of 10, and thus a high power factor and figure of merit (zT). Using rigorous first-principles calculations of electron relaxation time, the estimated hole-doped and electron-doped zT of, respectively, 1.5 and 0.5 at 600 K is achieved for Al<small><sub>2</sub></small>Te<small><sub>5</sub></small>. The pioneering zT of Al<small><sub>2</sub></small>Te<small><sub>5</sub></small> compared to that of Al<small><sub>2</sub></small>Te<small><sub>3</sub></small> is rooted merely in its amorphous-like lattice thermal transport and its polytelluride chain. These findings underscore the importance of aluminum telluride and polymeric-based inorganic compounds as practical and cost-effective thermoelectric materials, pending further experimental validation.\",\"PeriodicalId\":99,\"journal\":{\"name\":\"Physical Chemistry Chemical Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":2.9000,\"publicationDate\":\"2024-06-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Chemistry Chemical Physics\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://doi.org/10.1039/d4cp01577k\",\"RegionNum\":3,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"CHEMISTRY, PHYSICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Chemistry Chemical Physics","FirstCategoryId":"92","ListUrlMain":"https://doi.org/10.1039/d4cp01577k","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
Polytelluride square planar chain induced anharmonicity results in ultralow thermal conductivity and high thermoelectric efficiency in Al2Te5 monolayers
Two-dimensional (2D) metal chalcogenides provide rich ground for the development of nanoscale thermoelectrics, although achieving optimal thermoelectric efficiency has yet to be a challenge. Here, we leverage the unique chemistry of tellurium (Te), renowned for its hypervalent bonding and catenation abilities, to tackle this challenge as manifested in Al2Te3 and Al2Te5 monolayers. While the former forms a straightforward covalent Al–Te network, the latter adopts a more intricate bonding mechanism, enabled by eccentric features of Te chemistry, to maintain charge balance. In Al2Te5, a square planar chain (SPC) known as polytelluride [Te3]2- is neutralized by covalently bonded [Al2Te2]2+ framework. The hypervalent nature of Te results in bizarre Born effective charges of 7 and -4 for adjacent Te atoms within the square planar chain, the feature that induces significant anharmonicity, and leads to a glass-limit of lattice thermal conductivity (κL) in Al2Te5 monolayers. Enhanced anharmonic lattice vibrations and the accordion pattern bestow glass-like, strongly anisotropic thermal conductivity to the Al2Te5 monolayer. The calculated κL values of 1.8 and 0.5 Wm-1K-1 along the a- and b-axes at 600 K are one order of magnitude lower than those of Al2Te3, and even lower than monolayers that contain heavy cations like Bi2Te3. Moreover, the tellurium chain dominates the valence band maximum and conduction band minimum of Al2Te5, leading to a high valley degeneracy of 10, and thus a high power factor and figure of merit (zT). Using rigorous first-principles calculations of electron relaxation time, the estimated hole-doped and electron-doped zT of, respectively, 1.5 and 0.5 at 600 K is achieved for Al2Te5. The pioneering zT of Al2Te5 compared to that of Al2Te3 is rooted merely in its amorphous-like lattice thermal transport and its polytelluride chain. These findings underscore the importance of aluminum telluride and polymeric-based inorganic compounds as practical and cost-effective thermoelectric materials, pending further experimental validation.
期刊介绍:
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